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Metal coordination with an amide-functionalized axially chiral resorcinarene Jamila Vaughan,a Munna Ali Mohamed Bertata,a,b Brian W. Skelton,c Mark I. Ogden,a and Mauro
Mocerinoa,*
a Curtin Institute for Functional Molecules and Interfaces, School of Molecular and Life Science, Curtin University, GPO Box U 1987, Western Australia 6845 b Faculty of Science, University of Sebha, Libya c School of Molecular Sciences, University of Western Australia, Perth, Western Australia 6009, Australia. email: [email protected] Abstract The synthesis and characterization of an amide-functionalized axially chiral resorcinarene,
14,36,56,76-tetra-2-oxo-2-(2-hydroxyethylamino)ethoxy-16,34,54,74-tetramethoxy-2,4,6,8-
tetrapropylresorcin[4]arene, is reported. Metal complexation with picrate salts gave crystalline
products that could be structurally characterised for calcium, lanthanum, praseodymium, and
ytterbium. While the details of these structures vary, the metal-ligand interactions are remarkably
consistent, with coordination polymers formed through interaction between three of the amide O
atoms, each binding to a different metal atom. No other potential donor atom of the macrocycle is
bound to the metal atoms, with the coordination spheres completed by solvent or picrate donor O
atoms.
Keywords: resorcinarene, lanthanide, picrate, crystal structure
Dedicated to Prof. Karsten Gloe on the occasion of his 70th birthday.
2
Introduction
Resorcinarenes are macrocyclic compounds derived from resorcinol subunits that have attracted a
great deal of attention in supramolecular chemistry. Amongst the many different approaches to
functionalise these compounds, asymmetric functionalisation with achiral moieties to produce chiral
molecules1 has been of interest to our group,2-4 and others.5-9 The single step synthesis of the
axially-chiral tetramethoxy derivative provided ready access to a racemic mixture (Figure 1).4
Resolution was later achieved by conversion to a tetracamphorsulfonate derivative followed by
separation of the diastereomers by column chromatography, and hydrolysis to afford the
enantiomerically-pure axially-chiral tetramethoxy-resorcinarene.7 Further derivatization of these
products through Mannich reactions, and alkylation of the phenol O atoms has provided receptors
useful for ligand-assisted reactions.5, 6
Figure 1 One-step synthesis of the axially-chiral resorcinarene, 1.4
We have previously reported the synthesis of C4-symmetric pyridine-substituted resorcinarenes
through direct alkylation of 1, isolated as racemic mixtures, which were investigated as potential
metal-binding receptors. A copper complex was structurally characterised and found to form a
linear coordination polymer.2 Yan et al., has reported the synthesis, crystal structures and
complexing propertiesof tetramethoxyresorcinarene derivatives functionalized with
tetraacylhydrazones.(Ref 15). The complexing properties of the ligands towards a range of
transition metals and lead(II) were studies by monitoring changes in UV-Vis spectra. Crystal
structures of the metal complexes were not reported. In a subsequent paper, Yan et al., reported the
fluorescence sensing properties of these ligands. (Ref 16) The found that the salicylaldehyde
derived Shiff bases showed efficient recognition of zinc ions with a remarkable enhancement of
fluorescence intensity. We have now extended our work by functionalising the resorcinarene with
an hydroxyethylamide donor group to form racemic L (Figure 2), with the aim of binding harder
metal ions, such as Group 2, and lanthanoid cations. We report here the synthesis of L, along with
the intermediate tetraester 2, which we have described previously as a corrosion inhibitor.10 We also
BF3.Et2ODCM, RT, 2h
OHMeO
HO
MeO
HO OMe
OH
OMePr Pr
PrPr
HO OMe
OH
OMe
OHMeO
HO
MeOPrPr
Pr Pr
OHMeO
O
HPr
+
3
report crystal structures of the calcium, lanthanum, praseodymium, and ytterbium complexes of L
isolated as picrate salts.
Figure 2 Structures of resorcinarene ester intermediate 2, and the target ligand, L
Experimental
Chemical reagents and solvents were purchased from Sigma-Aldrich. Calcium picrate
pentahydrate,11 lanthanoid picrate hydrates (Ln = La, Pr, Yb),12, 13 and 2,4,6,8-tetrapropyl-
16,34,54,74-tetramethoxyresorcin[4]arene-14,36,56,76-tetrol 1,4 were synthesised by literature
methods. Melting points were recorded on a VWR-IA9100 instrument using open ended capillaries.
Infrared spectra (IR) were collected using FTIR-ATR, on a Perkin-Elmer Spectrum TwoTM
Infrared Spectrometer. Nuclear Magnetic Resonance (1H, DEPT-Q 13C, 2D COSY, 2D HSQC, 2D
HMBC) spectra were obtained using a Bruker Ultrashield 400TM instrument (400 MHz) at room
temperature. Chemical shifts were recorded on the δ scale relative to the deuterated solvent (CDCl3,
DMSO).
Synthesis
14,36,56,76-tetraethoxycarbonylmethyleneoxy -16,34,54,74-tetramethoxy-2,4,6,8-
tetrapropylresorcin[4]arene, 2
Resorcinarene 1 (5.02 g, 7.04 mmol), ethyl bromoacetate (10.0 g, 0.06 mol) and potassium
carbonate (15.37 g, 0.11 mol) were dissolved in dry acetonitrile (100 mL) and heated at reflux
overnight. The reaction mixture was then cooled, filtered and the remaining ethyl bromoacetate and
acetonitrile were removed at reduced pressure yielding a white precipitate which was dissolved in
2 L
OMeO
O
MeO
O OMe
O
OMePr Pr
PrPr
OEt
O
O
OEt
EtO
O
OEt
O
OMeO
O
MeO
O OMe
O
OMePr Pr
PrPr
HN
O
O
NH
HN
O
NH
O
HO
OH
OH
HO
4
ethyl acetate (20 mL) and washed with water (2 x 100 mL) and brine (1 x 100 mL). The organic
layer was dried with magnesium sulfate and the ethyl actetate was removed under reduced pressure
leaving a glass like oil which was recrystallised from ethanol yielding white crystals (4.6 g, 61%
yield, mp 133 °C). 1H NMR CDCl3 δ 0.91 (t, J = 7.2 Hz, 12 H, CH2CH3). 1.27 (t, J = 7.1 Hz, 12H,
OCH2CH3), 1.30 – 1.39 (apparent q, 8H, CH2CH3), 3.60 (s, 12H, OCH3), 3.96, 4.20. (2d, J = 15.8
Hz, 8H, CH2CO), 4.21 - 4.26 (m, 12H, CH2O), 4.53 (t, J = 7.4 Hz, 4H, CHCH2), δ 6.28 (s, 4H, Ar
H), 6.61 (s, 4H, Ar H). 13C NMR (CDCl3) δ 14.22, 14.30 (2CH3), 21.08, 35.21, 37.00 (2CH2 and
CH), 55.56, 60.91, 68.37 (OCH3, OCH2CH3 and OCH2CO), 99.56, 126.27, 127.47, 128.20, 154.92,
155.85 (Ar), 169.6 (C=O). IR 1753 (CO), 2923 (CH2), 2855 (CH3), 1684 (C=C), 1301 cm-1 (C–O).
HRMS m/z [M+H]+ calculated for C60H81O16 1057.5535, found 1057.5502.
14,36,56,76-tetra-2-oxo-2-(2-hydroxyethylamino)ethoxy-16,34,54,74-tetramethoxy-2,4,6,8-
tetrapropylresorcin[4]arene, L
Compound 2 (1.05 g, 0.99 mmol) was dissolved in ethanolamine (20 mL, 0.33 mol) and heated at
reflux overnight. The reaction mixture was then acidified with HCl (200 mL, 5M) producing a light
green precipitate which was recrystallised from methanol yielding light green crystals of L (0.92 g,
86% yield, mp 222 °C). 1H NMR DMSO δ 0.86 (t, J = 7.4, Hz, 12H, CH3CH2), 1.15 – 1.89 (m, 8H,
CH2CH3), 1.70 – 1.88 (m, 8H, CH2CH), 3.13 -3.33 (m, 8H, CH2N), 3.39 – 3.48 (m, 8H, CH2OH),
3.65 (s, 12H, OCH3), 4.10, 4.24. (2d, J = 14.6 Hz, 8H, CH2CO), 4.48 (t, J = 7.4 Hz, 4H, OH), 4.83
(t, J = 5.3 Hz, 4H, CHCH2), 6.52 (s, 4H, Ar), 6.74 (s, 4H, Ar), 7.33 (t, J = 5.7 Hz, 4H, NH). 13C
NMR. (DMSO) δ 14.52 (CH3), 21.20, 34.64, 37.28, (2CH2, CH), 41.60, 56.47 (CH2OH, CH2N),
60.12, 68.31 (CH2O and CH3O), 98.50, 125.19, 125.71, 126.18, 154.14, 155.64 (Ar), 168.42 (CO).
IR 3372 cm-1 (NH), 1655 cm-1 (C=O). HRMS, [M+H]+ calculated for C76H121N8O12, 1117.5884
m/z, found, 1117.5925 m/z.
Metal complexation with L
The required metal picrate hydrate (Ca, La, Pr, or Yb, ~2 mg, excess) and L (2 mg, XX mmol) were
dissolved in 1:1 dichloromethane:methanol (1-2 mL). The resulting solution was filtered, and
allowed to evaporate under ambient conditions resulting in the deposition of highly efflorescent
orange crystals in variable yield. These were subjected to single crystal X-ray analysis.
Structure Determinations
Crystallographic data for the structures were collected at 100(2) K on an Oxford Diffraction Gemini
diffractometer using Mo Kα radiation. Following multi-scan absorption (analytical, for PrL)
corrections, the structures were refined against F2 with full-matrix least-squares using the program
5
SHELXL-2017.14 Anisotropic displacement parameters were employed for all the non-hydrogen
atoms, unless otherwise stated. H-atoms were added at calculated positions and refined by use of a
riding model with isotropic displacement parameters based on those of the parent atom, unless
otherwise stated.
Refinement details L·MeOH: The atoms of the hydroxyethylamine part -NH(CH2)2OH of one chain (43n) were found
to be disordered over two sets of sites with occupancies refining to 0.626(2) and its complement for
the two components. Another hydroxyl group (33n) and each of the three methanol solvent
molecules were also found to be disordered over two sites with occupancies for each of their two
components constrained be the same as those for the 43n chain on the basis of close contacts and
trial refinement. The hydroxyl group on chain 13n was also found to be disordered over two sets of
sites with occupancies constrained to be equal for the two components after trial refinement.
Hydrogen atoms on the oxygen atoms of the disordered solvent methanol molecules were not
located.
CaL: Some atoms of two of the chains, 13n and 23n, were modelled as being disordered over two
sets of sites. Occupancies for the two components of the atoms 13n were set to be the same after
trial refinement found them not to be significantly different. Those for the two components of 23n
refined to 0.752(6) and its complement. Geometries of the disordered atoms of 13n were restrained
to ideal values. Hydrogen atoms on the hydroxyl groups of the disordered ligands and those on the
water molecules were not located.
LaL: The terminal atom of one n-propyl chain, 31n, and the terminal C and O atom of one long
chain, 43n, were all modelled as being disordered over two positions. The site occupancies of
C(213) and C(214) were refined to 0.655(11) and its complement. Those for the other disordered
chain were set at 0.5 after trial refinement. Hydroxyl hydrogen atoms H(134) and H(334) were
refined without restraints. Coordinated water molecule hydrogen atoms were located and refined
with restrained geometries. Two solvent water molecules were assigned occupancies of 0.5 after
trial refinement and refined with isotropic displacement parameters.
PrL: Some atoms of two of the long chains were modelled as being disordered over two sets of
sites. The site occupancies of the two sets of atoms of chain 13n were set to be equal after trial
refinement found them not to be significantly different. The occupancies of the two sets of atoms
for chain 43n were refined to 0.741(2) and its complement. The picrate anion was also found to be
disordered over two sets of sites with occupancies constrained to be the same as those for chain 43n
on the basis of close contacts. The two solvent molecules associated with these disordered groups
6
were modelled as a MeOH and a water molecule and were also refined with the same occupancy
factors on the basis of close intermolecular contacts. Remaining solvent molecules were modelled
as methanol molecules with unit occupancies set after trial refinement. Geometries of the disordered
atoms were restrained to ideal values. Hydroxyl hydrogen atoms of the disordered chains and those
on the coordinated and solvent water molecules were not located or easily inferred on the basis of
hydrogen bonding contacts as a result of disordered donor or acceptor groups.
YbL: Some atoms of two of the long chains and one propyl chain were modelled as being
disordered over two sets of sites with occupancies set to be the same for each group after trial
refinement found them not to be significantly different. Solvent molecules were modelled as water
or methanol molecules with occupancies set at one or 0.5 after trial refinement. Geometries and
displacement parameters of the long chains and of the disordered atoms were restrained to
acceptable values. The coordinated picrate was also modelled as being disordered with site
occupancies constrained to 0.5. Geometries were restrained to ideal values. Solvent water molecule
and hydroxyl hydrogen atoms were located where possible according to hydrogen bonding
interactions. Those hydrogen atoms on disordered oxygen atoms were not included due to several
possible sites. The electron density which could not be easily modelled as solvent was effectively
removed by use of the program SQUEEZE. The disordered solvent molecules were refined with
isotropic displacement parameters.
Crystal and Refinement Data L·MeOH M = 1213.43, colourless block, 0.37 x 0.20 x 0.20 mm3, triclinic, space group P1̄ (No. 2),
a = 14.4690(4), b = 14.5206(4), c = 17.5110(4) Å, a = 107.453(2), b = 103.827(2), g = 104.551(2)°,
V = 3194.17(15) Å3, Z = 2, Dc = 1.262 g cm-3, µ = 0.093 mm-1. F000 = 1308, 2qmax = 65.51º, 67857
reflections collected, 21645 unique (Rint = 0.0277). Final GooF = 1.028, R1 = 0.0557, wR2 =
0.1560, R indices based on 14024 reflections with I > 2s(I) (refinement on F2), |Dr|max= 0.857 e Å-3,
926 parameters, 18 restraints. CCDC 1843155.
CaL M = 1772.78, orange plate, 0.20 x 0.16 x 0.04 mm3, triclinic, space group P1̄ (No. 2), a =
14.8360(7), b = 17.5063(9), c = 18.9380(10) Å, a = 112.083(5), b = 98.124(4), g = 104.631(4)°, V =
4254.1(4) Å3, Z = 2, Dc = 1.384 g cm-3, µ = 0.169 mm-1. F000 = 1878, 2qmax = 58.39º, 42304
reflections collected, 19674 unique (Rint = 0.0597). Final GooF = 0.905, R1 = 0.0739, wR2 =
0.1788, R indices based on 8088 reflections with I > 2s(I) (refinement on F2), |Dr|max= 1.463 e Å-3,
1163 parameters, 168 restraints. CCDC 1843329.
LaL M = 2048.64, orange plate, 0.28 x 0.22 x 0.06 mm3, monoclinic, space group P21/n (No. 14), a
= 14.3754(3), b = 36.0921(5), c = 18.8574(4) Å, b = 110.953(2)°, V = 9137.0(3) Å3, Z = 4, Dc =
7
1.489 g cm-3, µ = 0.570 mm-1. F000 = 4248, 2qmax = 60.0º, 115272 reflections collected, 26605
unique (Rint = 0.0574). Final GooF = 0.978, R1 = 0.0639, wR2 = 0.1758, R indices based on 16984
reflections with I > 2s(I) (refinement on F2), |Dr|max= 6.391 e Å-3, 1274 parameters, 44 restraints.
CCDC 1843723.
PrL M = 2085.21, orange slab, 0.35 x 0.25 x 0.13 mm3, triclinic, space group P1̄ (No. 2), a =
13.6762(4), b = 20.1867(5), c = 20.4351(5) Å, a = 110.659(2), b = 98.306(2), g = 109.547(3)°, V =
4749.1(2) Å3, Z = 2, Dc = 1.458 g cm-3, µ = 0.612 mm-1. F000 = 2168, 2qmax = 68.99º, 110917
reflections collected, 37374 unique (Rint = 0.0427). Final GooF = 0.973, R1 = 0.0507, wR2 =
0.1285, R indices based on 25818 reflections with I > 2s(I) (refinement on F2), |Dr|max= 1.949 e Å-3,
1447 parameters, 232 restraints. CCDC 1896385.
YbL M = 2058.77, yellow plate, 0.28 x 0.12 x 0.05 mm3, triclinic, space group P1̄ (No. 2), a =
14.4892(9), b = 19.7037(17), c = 19.7502(16) Å, a = 60.988(9), b = 75.313(6), g = 70.328(7)°, V =
4615.2(6) Å3, Z = 2, Dc = 1.481 g cm-3, µ = 1.111 mm-1. F000 = 2124, 2qmax = 57.36º, 47344
reflections collected, 20494 unique (Rint = 0.0811). Final GooF = 0.941, R1 = 0.0877, wR2 =
0.1995, R indices based on 9360 reflections with I > 2s(I) (refinement on F2), |Dr|max= 2.570 e Å-3,
1356 parameters, 485 restraints. CCDC 1896384.
Supplementary material Full details of the structure determinations have been deposited with the Cambridge
Crystallographic Data Centre as CCDC 1843155, 1843329, 1843723, 1896384, 1896385. These
data can be obtained free of charge via http://www.ccdc.cam.ac.uk/conts/retrieving.html, or from
the Cambridge Crystallographic Data Centre, 12 Union Road, Cambridge CB2 1EZ, UK; fax: (+44)
1223-336-033; or e-mail: [email protected].
Results and Discussion
Ligand Synthesis and Characterisation
The ligand L, was synthesized in two steps from resorcinarene 1 using modifications of established
methods. Alkylation of 1 with ethyl bromoacetate using the procedure described by Buckley et al.6
gave the required tetraester 2 in moderate yield. In addition to the standard characterisation
techniques, a single crystal structure determination of this compound was carried out (see
Supplementary Information). Aminolysis of tetraester was achieved by heating 2 in excess
ethanolamine at reflux. This gave the required hydroxamide in moderate yield as a crystalline solid.
8
Yan's group has reported a similar aminolysis reaction of the methyl esters derivatives using
hydrazine15 and ethylenediamine16 and also reported crystal structures of the resulting ligands.
In a number of cases, the ligand crystallised in the presence of metal salts forming crystals
appropriate for single crystal X-ray structure determination. These were found to be a methanol
solvate (L·MeOH) in one case, and a hydrate (L·H2O) in another, although there was no deliberate
change in the experimental procedure. It is assumed variations in the evaporation rate and specific
concentrations influence the crystallization process. Neither of these structures were of sufficient
quality to locate all of the protons, and the macrocycle structure is similar in both, hence only
L·MeOH is discussed here. The data for L·H2O are given in the Supplementary Information.
Results of the structure determination confirmed the structure of L, with the compound crystallising
with three methanol solvent molecules. The molecular structure is shown in Figure 3, with the
macrocycle assuming the commonly observed “boat” conformation.17 The angles between the
pseudo 2-fold axis and the planes of each of the Ph rings are 81.73(4), 82.34(4)° (1n and 3n) and
3.23(4), 4.76(4)° (2n and 4n). The angle between opposite ‘vertical’ pairs is 15.94(5) (1n and 3n)
and 2.96(5)° (2n and 4n) between the ‘horizontal’ pairs.
Figure 3 Molecular structure of L·MeOH projected obliquely to the plane of the four CH groups. Only the atoms of
one or major component of the disordered components are shown. Ellipsoids have been drawn at the 50% probability
level.
9
Metal Complexes
Metal complexation was examined by adding metal picrate salts in excess to a
dichloromethane/methanol solution of L. The nature of the crystals deposited appeared to be
somewhat variable, presumably as a result of differing rates of evaporation, and possibly similar
solubilities of the ligand and metal complex. This resulted in the crystallization of free ligand in
some cases, as mentioned above. Nevertheless, it proved possible to obtain good quality crystals in
a number of cases, where the yellow picrate anion provided a simple indication that the metal was
likely to be present in the material.
CaL
The results of the structure determination of the calcium complex were consistent with a
formulation of {[CaL(OH2)(HOMe)(pic)](pic)·2H2O·3CH3OH}n. The complex forms a one-
dimensional polymer where one picrate anion is coordinated to the Ca atom and the second picrate
is not co-ordinated. The Ca is bonded to the oxygen atom of one of the amide chains and also two
other amide groups of two symmetry-related molecules, one related by an inversion centre and
another related by cell translations in the ab direction. The coordination sphere consists of the three
amide oxygen atoms, the oxygen bound picrate anion, one water molecule and one MeOH (Figure
4). The polymer is shown in Figure 5.
Figure 4 Molecular structure of CaL. The minor components of the disordered atoms and H atoms have been omitted.
Ellipsoids have been drawn at the 50% probability level.
10
Figure 5 The one-dimensional coordination polymer formed by CaL
The angles between the pseudo 2-fold axis and the planes of each of the Ph rings are
85.5(1), 85.2(1)° (1n and 3n) and 11.6(1), 14.2(1)° (2n and 4n). The angle between opposite
‘vertical’ pairs is 9.4(1) (1n and 3n) and 25.5(1)° (2n and 4n) between the ‘horizontal’ pairs.
There appears to be some interactions between the Ph ring (1n) and one of the coordinated
picrate anions (5n). The angle between the two rings is 4.0(1)° with the closest intra-molecular
distances being C(12)...N(54) 3.444(4), C(13)...N(54) 3.404(4) Å. The dihedral angle between the
two picrate rings is 15.6(1)° with the closest approaches being C(52)... O(621) 3.464(4),
C(53)...C(62) 3.351(5), and C(54)...C(62) 3.468(5) Å.
Although hydrogen atoms on the water molecules and on the hydroxyl groups of the
disordered chains were not located, others can be seen to form intra-and inter-molecular hydrogen
bonds. The amide hydrogen atom (H132, H135) forms an intra-molecular H-bond to the methoxy
oxygen atom on the neighbouring phenyl ring, with two of the others, H(232) and H(332),
interacting with an oxygen of a nitro-group and the phenolic oxygen of the uncoordinated picrate
anion. Of the two hydrogen atoms that were located on the ligand hydroxyl groups, one H(334),
hydrogen bonds to the coordinated water molecule of the molecule related by a symmetry
translation in the b direction thus linking the polymers. The other, H(434), bonds to an oxygen of
another nitro group of the uncoordinated picrate anion. The hydroxyl hydrogen atoms of the MeOH
molecules form H-bonds to either an uncoordinated water molecule (O(5)-H(5)...O(3)), the
uncoordinated picrate anion (O(6)-H(6)...O(61), O(6)-H(6)...O(621)) or a ligand hydroxyl oxygen
(O(7)-H(7)...O(434)). Details of the hydrogen bonded geometries are tabulated in the SI.
11
LaL
The results of the structure determination of the lanthanum complex were consistent with the
formulation {[LaL(OH2)4(pic)](pic)2·2H2O}n. The structure is similar to the CaL complex in terms
of the metal-L interactions, except that it is a two-dimensional polymer (Figure 6, Figure 7). Again
only one of the picrate anions is coordinated to the La atom, with the remaining two picrates not
coordinated. The coordination around the La consists of four water molecules, one picrate anion
bound through both the phenolic oxygen atom and a nitro group oxygen atom, and three ligand
carbonyl groups, one from the ligand in the asymmetric unit, one from a ligand generated by a
crystallographic 21 screw axis, and the third carbonyl from a ligand translated by one cell dimension
in the c direction. Hence, the metal is now nine coordinated, with the coordination geometry is best
described as a capped square antiprism as shown in Figure 8 where it is projected down the pseudo
4-axis.
Figure 6 Molecular structure of LaL . Hydrogen atoms and the minor components of the disordered atoms have been
omitted. Ellipsoids have been drawn at the 50% probability level.
12
Figure 7 The structure of LaL projected along the a axis showing its polymeric nature. Hydrogen atoms and the minor
components of the disordered atoms have been omitted.
Figure 8 The 9-coordinate capped square antiprism coordination sphere of LaL projected approximately down the O(4)-
La(1) bond (the pseudo 4 axis). The superscripts refer to the atoms generated by the 21 screw (1) and the cell translation
(2).
The angles between the pseudo 2-fold axis and the planes of each of the Ph rings are
91.08(8), 89.13(8)° (1n and 3n) and 17.73(8), 12.47(8)° (2n and 4n). The angle between opposite
‘vertical’ pairs is 2.1(1) (1n and 3n) and 30.1(1)° (2n and 4n) between the ‘horizontal’ pairs.
13
As observed in the CaL complex, there appears to be some interactions between the Ph ring
(1n) and the coordinated picrate anions (5n). The angle between the two rings is 3.6(1)° with the
closest intra-molecular distances being C(13)...N(54) 3.396(4), C(14)...C(54) 3.454(4), and
O(13)...O(541) 3.380(3) Å. There also appears to be interactions between the coordinated and one
uncoordinated picrate with the interplanar angle being 2.9(1)°. Closest approaches are
O(522)...N(76) 3.132(4), C(55)...O(722) 3.231(4), C(56)...O(722) 3.209(4), N(56)...O(722) 3.099(4)
Å.
Three of the four amide NH groups are involved in intra-molecular hydrogen bonds to the
methoxy oxygen atoms on the neighbouring Ph rings. The H...O distances lie in the range 2.17 -
2.19 with the N-H...O angles ranging from 143.9 to 150.4°. The alcohol groups form hydrogen
bonds to picrate anions, water molecules or in the case of H(334) to the alcohol oxygen atom
O(134) of the molecule generated by the crystallographic n glide plane. The coordinated water
molecule O(2) forms an intramolecular hydrogen bond to the coordinated picrate, H(2AO)...O(561)
2.197(19) Å, O(2)-H(2AO)...O(561) 174(4)°. There are also hydrogen bonds between the
coordinated water molecules and the uncoordinated picrate anions, the solvent water molecules and
also between O(4) and the amide oxygen atom O(132) and also between O(1) and the alcohol
oxygen atom O(334). Details are tabulated in the SI.
PrL
The results of the structure determination of the praseodymium complex were consistent with the
formulation {[PrL(OH2)(HOMe)(pic)2](pic)·0.25H2O·2.75CH3OH}n.(Figure 9, Figure S4) The
structure is similar to the previous two complexes in terms of metal-L interactions, in this case
forming a one-dimensional polymer where two of the three picrate anions are coordinated to the Pr
atom with the third picrate not coordinated. The coordination around the Pr consists of one water
molecule, one methanol molecule, two picrates both bound through the phenolic oxygen atom and a
nitro group, and three ligand carbonyl groups, one from the ligand of the asymmetric unit, one from
a ligand generated by a crystallographic inversion centre creating a centrosymmetric dimer (see
Figure 9) and the third carbonyl from a ligand translated by one cell dimension in the b direction.
The metal is thus nine coordinated, but with a much different ligand set compared to LaL. The
geometry is best described as a capped square antiprism as shown in Figure 10 projected down the
pseudo 4-axis.
14
Figure 9 Molecular structure of PrL projected approximately onto the plane of the four (CH) groups showing the
dimeric component of the polymer. The minor components of the disordered atoms and hydrogen atoms have been
omitted.
15
Figure 10 The 9-coordinate capped square antiprism coordination sphere of PrL projected approximately down the
O(5)-Pr(1) bond (the pseudo 4 axis). The ‘ refers to the atom generated by 1-x,2-y,1-z with “ referring to the atom
generated by 1+x,1+y,z.
The angles between the pseudo 2-fold axis and the planes of each of the Ph rings are
85.06(5), 87.35(5)° (1n and 3n) and 18.63(5), 15.91(5)° (2n and 4n). The angle between opposite
‘vertical’ pairs is 7.61(7) (1n and 3n) and 34.37(7)° (2n and 4n) between the ‘horizontal’ pairs.
As was observed in the previous complexes, there appears to be some interactions between
the Ph ring (1n) and one of the coordinated picrate anions (6n). The angle between the two rings is
4.08(7)° with the closest intra-molecular distances being C(13)...N(64) 3.354(3), C(14)...C(64)
3.383(3), and O(13)...O(641) 3.272(3) Å. The two coordinated picrate anions have a dihedral angle
between the rings of 90.12(8)°.
Although hydrogen atoms were not located for the coordinated water molecule, some
hydrogen interactions are observed. Two of the amide NH groups are involved in intra-molecular
hydrogen bonds to methoxy oxygen atoms, the remaining two forming interactions to a solvent
methanol molecule or the nitro group of the uncoordinated picrate group. As a result of the disorder,
only two of the ligand hydroxyl hydrogen atoms were observed. One of these H(234) forms
hydrogen bonds to carbonyl oxygen atom O(232) of the molecule related by an inversion centre
with the hydrogen atom of the other hydroxyl H(334) forming hydrogen bonds to an oxygen atom
16
of a nitro group of the uncoordinated picrate anion (O(741)/O(871)). Solvent methanol hydroxyl
hydrogen atoms form hydrogen bonds to the coordinated hydroxyl group (H(5O)...O(234) 2.07Å),
another methanol molecule (H(7)...O(8) 1.88 Å), and the uncoordinated picrate anion
(H(6O)...O(8), H(7)...O(842) Å). Details are tabulated in the SI.
YbL
The results of the structure determination of the ytterbium complex were consistent with the
formulation {[YbL(OH2)(pic)2](pic)·H2O·1.5CH3OH}n. (Figure 11) The structure consisting of a
one-dimensional polymer where two of the three picrate anions are coordinated to the Yb atom with
the third picrate not coordinated. The coordination around the Yb therefore consists of one water
molecule, two picrates both bound through the phenolic oxygen atom and a nitro group, and three
ligand carbonyl groups, one from the ligand in the asymmetric unit, one from a ligand generated by
a crystallographic inversion centre creating a centrosymmetric dimer (see Figure 12) and the third
carbonyl from a ligand translated by one cell dimension in the b direction. The metal is now eight
coordinated, compared to nine coordinate for LaL and PrL, consistent with the smaller size of the
Yb cation. The geometry is best described as a square antiprism as shown in Figure 13 projected
down the pseudo 4-axis. The polymer is shown in Figure 14.
The angles between the pseudo 2-fold axis and the planes of each of the Ph rings are
83.1(2), 84.9(3)° (1n and 3n) and 6.7(2), 8.5(2)° (2n and 4n). The angle between opposite ‘vertical’
pairs is 12.2(3) (1n and 3n) and 15.2(3)° (2n and 4n) between the ‘horizontal’ pairs.
Again, a common feature is apparent interaction between the Ph ring (1n) and one of the
coordinated picrate anions (6n). The angle between the two rings is 5.8(3)° with the closest intra-
molecular distances being C(12)...N(64) 3.33(1), C(13)...O(642) 3.36(1), C(14)...C(65) 3.25(1), and
O(15)...C(66) 3.240(9) Å. The dihedral angle between the two coordinated picrate rings is much
less than that observed in PrL at 31.5(5)°.
17
Figure 11 Molecular structure of YbL . Hydrogen atoms and the minor components of the disordered atoms have been
omitted. Ellipsoids have been drawn at the 30% probability level.
18
Figure 12 Molecular structure of YbL projected approximately onto the plane of the four (CH) groups showing the
dimeric component of the polymer. The minor components of the disordered atoms and hydrogen atoms have been
omitted.
Figure 13 The 8-coordinate square antiprism coordination sphere of YbL projected approximately down the pseudo 4
axis. The ‘ refers to the atom generated by 1-x,1-y,1-z with “ referring to the atom generated by x,y-1,z.
19
Figure 14 The one-dimension polymer of YbL projected down the a axis.
Structural Comparisons
A remarkable aspect of these structure determinations is the consistent nature of the interactions
between L and the various metal cations. In each case, the metal is bound to three amide O atoms,
all from different L molecules, resulting in the formation of coordination polymers. The fourth
amide O atom is left uncoordinated in each of the structures. That calcium should form a similar
complex to lanthanoid complexes is consistent with the use of lanthanoids as calcium substitutes in
biological systems.18 Structural similarities have previously been observed in the 1:1 calcium and
europium complexes of p-t-butylcalix[8]arene.19 Simplified views of the macrocycle conformation
and disposition of the three bound metal cations are shown for each of the complexes in Figure 15.
CaL, PrL, and YbL are all very similar, consistent with their formation of one-dimensional
coordination polymers. LaL differs somewhat in the disposition of the metal cations, and forms a
two-dimensional polymer. It is possible that the consistent nature of these structures is also
significantly impacted by the use of the picrate anion, with interactions between aromatic rings of
the calixarene and picrate anions being observed in each case. Further work using different
precursor metal salts will be required to further investigate this behavior.
20
(a)
(b)
(c)
(d)
Figure 15 Simplified views emphasising the macrocycle conformation and metal-O(amide) interactions for (a) CaL, (b) LaL, (c) PrL, and (d) YbL.
References
1. McIldowie, M. J.; Mocerino, M.; Ogden, M. I., A brief review of C-n-symmetric calixarenes and resorcinarenes. Supramol Chem 2010, 22 (1), 13-39.
2. McIldowie, M. J.; Mocerino, M.; Ogden, M. I.; Skelton, B. W., Pyridine-functionalised C-4 symmetric resorcinarenes. Tetrahedron 2007, 63 (44), 10817-10825.
3. McIldowie, M. J.; Mocerino, M.; Ogden, M. I.; Skelton, B. W.; White, A. H., C-4 Dissymmetric resorcinarene derivatives: synthesis, crystal structure and micelle formation. J Incl Phenom Macro 2015, 82 (1-2), 47-51.
4. McIldowie, M. J.; Mocerino, M.; Skelton, B. W.; White, A. H., Facile Lewis acid catalyzed synthesis of C-4 symmetric resorcinarenes. Org Lett 2000, 2 (24), 3869-3871.
5. Buckley, B. R.; Boxhall, J. Y.; Page, P. C. B.; Chan, Y.; Elsegood, M. R. J.; Heaney, H.; Holmes, K. E.; McIldowie, M. J.; Mckee, V.; McGrath, M. J.; Mocerino, M.; Poulton, A. M.; Sampler, E. P.; Skelton, B. W.; White, A. H., Mannich and O-alkylation reactions of tetraalkoxyresorcin[4]arenes - The use of some products in ligand-assisted reactions (pg 5117, 2006). Eur J Org Chem 2007, (7), 1203-1203.
6. Buckley, B. R.; Boxhall, J. Y.; Page, P. C. B.; Chan, Y. H.; Elsegood, M. R. J.; Heaney, H.; Holmes, K. E.; McIldowie, M. J.; McKee, V.; McGrath, M. J.; Mocerino, M.; Poulton, A. M.; Sampler, E. P.; Skelton, B. W.; White, A. H., Mannich and O-alkylation reactions of tetraalkoxyresorcin[4]arenes - The use of some products in ligand-assisted reactions. Eur J Org Chem 2006, (22), 5117-5134.
7. Buckley, B. R.; Page, P. C. B.; Chan, Y.; Heaney, H.; Klaes, M.; McIldowie, M. J.; McKee, V.; Mattay, J.; Mocerino, M.; Moreno, E.; Skelton, B. W.; White, A. H., The preparation and absolute configurations of enantiomerically pure C-4-symmetric tetraalkoxyresorcin[4]arenes obtained from camphorsulfonate derivatives. Eur J Org Chem 2006, (22), 5135-5151.
8. Salorinne, K.; Nissinen, M., Novel tetramethoxy resorcinarene bis-crown ethers. Org Lett 2006, 8 (24), 5473-5476.
21
9. Tero, T. R.; Suhonen, A.; Salorinne, K.; Campos-Barbosa, H.; Nissinen, M., The Missing Member of the Partially O-Alkylated Resorcinarene Family: Synthesis and Conformation of Methyl Tetramethoxy Resorcinarene. Org Lett 2013, 15 (5), 1096-1099.
10. Tan, Y. J.; Mocerino, M.; Paterson, T., Organic molecules showing the characteristics of localised corrosion aggravation and inhibition. Corros Sci 2011, 53 (5), 2041-2045.
11. Diakiw, V.; Hambley, T. W.; Kepert, D. L.; Raston, C. L.; White, A. H., Crystal-Structure of Calcium Picrate Pentahydrate - New 8-Coordinate Stereochemistry for [M(Bidentate)2(Unidentate)4]. Aust J Chem 1979, 32 (2), 301-309.
12. Harrowfield, J. M.; Lu, W. M.; Skelton, B. W.; White, A. H., Structural Systematics of Rare-Earth Complexes .1. Structural Characterization of Lanthanoid(III) Picrate Hydrates - Monoclinic (P21/c) (Quasi-)Dodecahydrates of the Related La -] Pr and Nd -] Tb Families. Aust J Chem 1994, 47 (2), 321-337.
13. Harrowfield, J. M.; Lu, W. M.; Skelton, B. W.; White, A. H., Structural Systematics of Rare-Earth Complexes .2. Structural Characterization of Lanthanoid(III) Picrate Hydrates - the Triclinic , 11.5 Hydrates of the Later Rare-Earths and Yttrium. Aust J Chem 1994, 47 (2), 339-348.
14. Sheldrick, G. M., Crystal structure refinement with SHELXL. Acta Crystallogr C 2015, 71, 3-8.
15. Sun, J.; Zhang, L. L.; Yao, Y.; Yan, C. G., Synthesis, crystal structures and complexing properties of tetramethoxyresorcinarene functionalized tetraacylhydrazones. J Incl Phenom Macro 2014, 79 (3-4), 485-494.
16. Li, L.; Sun, J.; Zhang, L. L.; Yao, R.; Yan, C. G., Crystal structure and fluorescence sensing properties of tetramethoxyresorcinarene functionalized Schiff bases. J Mol Struct 2015, 1081, 355-361.
17. Puttreddy, R.; Beyeh, N. K.; Rissanen, K., Conformational changes in C-methyl-resorcinarene pyridine N-oxide inclusion complexes in the solid state. Crystengcomm 2016, 18 (26), 4971-4976.
18. Hewitt, S. H.; Butler, S. J., Application of lanthanide luminescence in probing enzyme activity. Chem Commun 2018, 54 (50), 6635-6647.
19. Harrowfield, J. M.; Ogden, M. I.; Richmond, W. R.; White, A. H., Lanthanide Ions as Calcium Substitutes - a Structural Comparison of Europium and Calcium Complexes of Ditopic Calixarene. J Chem Soc Dalton 1991, (8), 2153-2160.
1P
Metal coordination with an amide-functionalized axially chiral resorcinarene Jamila Vaughan, Munna Ali Mohamed Bertata, Brian W. Skelton, Mark I. Ogden, and Mauro Mocerino*
Supplementary Information
Crystal Structure of 14,36,56,76-tetraethoxycarbonylmethyleneoxy -16,34,54,74-tetramethoxy-2,4,6,8- tetrapropylresorcin[4]arene, 2 ........................................................ 2
Crystal structure of 14,36,56,76-tetra-2-oxo-2-(2-hydroxyethylamino)ethoxy-16,34,54,74-tetramethoxy-2,4,6,8- tetrapropylresorcin[4]arene, L·3H2O ............................................... 4
Additional details for the structure of CaL ........................................................................... 6
Additional details for the structure of LaL ............................................................................ 8
Additional details for the structure of PrL .......................................................................... 11
Additional details for the structure of YbL ......................................................................... 15
Crystal Structure of 14,36,56,76-tetraethoxycarbonylmethyleneoxy -16,34,54,74-tetramethoxy-2,4,6,8- tetrapropylresorcin[4]arene, 2 A crystal of 2 was grown by slow evaporation of an ethanol solution, and was characterised by single crystal X-ray crystallography. The crystal data for 2 are summarized in Table S1 with the structure depicted in Figs. S1 and S2 where ellipsoids have been drawn at the 50% probability level. Crystallographic data for the structures were collected at 100(2) K on an Oxford Diffraction Gemini diffractometer using Mo Kα radiation. Following multi-scan absorption corrections, the structure was refined against F2 with full-matrix least-squares using the program SHELXL-2017.1 One ethoxycarbonylmethoxy group was modelled as being disordered over two sets of sites with sites occupancies refined to 0.835(4) and its complement. The methyl group of the methoxy group on the opposite Ph ring was also modelled as being disordered over two sets of sites, with occupancies refined to 0.744(7) and its complement. All H-atoms were added at calculated positions and refined by use of a riding model with isotropic displacement parameters based on those of the parent atom. Anisotropic displacement parameters were employed for all the non-hydrogen atoms. Full details of the structure determinations for 2 have been deposited with the Cambridge Crystallographic Data Centre as CCDC 1842968. Table S1. Crystal data and structure refinement for 2. Empirical formula C60H80O16 Formula weight 1057.24 Temperature 100(2) K Wavelength 0.71073 Å Crystal system Monoclinic Space group P21/n Unit cell dimensions a = 12.2429(4) Å b = 12.2968(5) Å c = 37.255(3) Å b= 91.459(4)° Volume 5606.9(5) Å3 Z 4 Density (calculated) 1.252 Mg/m3 μ 0.090 mm-1 F(000) 2272 Crystal size 0.36 x 0.19 x 0.11 mm3 θ range for data collection 3.531 to 30.517°. Index ranges -16<=h<=16, -17<=k<=13, -30<=l<=52 Reflections collected 36878 Independent reflections 15395 [R(int) = 0.0437] Completeness to θ= 25.242° 99.7 % Absorption correction Semi-empirical from equivalents Max./min. transmission 1.00/ 0.976 Refinement method Full-matrix least-squares on F2 Data / restraints / parameters 15395 / 53 / 734 Goodness-of-fit on F2 0.832 Final R indices [I>2σ(I)] R1 = 0.0476, wR2 = 0.0932 R indices (all data) R1 = 0.0990, wR2 = 0.1010 Largest diff. peak and hole 0.410 and -0.342 e.Å-3
Fig. S1 Molecular structure of 2 . Only one set of disordered atoms is shown. Hydrogen atoms have been omitted.
Fig. S2 Molecular structure of 2 projected approximately onto the plane of the four (CH) groups. Only one set of disordered atoms is shown. Hydrogen atoms have been omitted.
Crystal structure of 14,36,56,76-tetra-2-oxo-2-(2-hydroxyethylamino)ethoxy-16,34,54,74-tetramethoxy-2,4,6,8- tetrapropylresorcin[4]arene, L·3H2O The crystal data for L·3H2O are summarized in Table S2 with the structure depicted in Fig. S3 where ellipsoids have been drawn at the 30% probability level. Crystallographic data for the structures were collected at 100(2) K on an Oxford Diffraction Gemini diffractometer using Cu Kα radiation. Following solution by direct methods and multi-scan absorption corrections, the structure was refined against F2 with full-matrix least-squares using the program SHELXL-2017.1 The terminal oxygen atoms of three of the four hydroxylethanolamide chains were each modelled as being disordered over two sets of sites with occupancies set at 0.5 after trial refinement. The terminal two atoms on the nPr chain, C(31n), were also modelled as disordered with occupancies set at 0.5. The occupancies of the water molecules O1-O5 were constrained to 1.0 or 0.5 from trial refinement. Hydrogen atoms on the disordered hydroxylethanolamide chains and disordered solvent water molecules were not located nor could their positions be readily determined from possible hydrogen bonding interactions. Hydrogen atoms for water molecule O1 and for O234 were included at positions suitable for hydrogen bonding and refined with geometrical restraints. Geometries involving the disordered atoms were restrained to ideal values. Anisotropic displacement parameters were employed for all non-hydrogen atoms. All remaining H-atoms were added at calculated positions and refined by use of a riding model with isotropic displacement parameters based on those of the parent atom. Table S3 lists the hydrogen bonding for those hydrogen atoms which could be located. Full details of the structure determinations for L·3H2O have been deposited with the Cambridge Crystallographic Data Centre as CCDC 1896386.
Fig. S3 Molecular structure of L·3H2O projected approximately onto the plane of the four CH groups. Only the atoms of one, or major, component of the disorder are shown.
Table S2. Crystal data and structure refinement for L·3H2O. Empirical formula C60H9N4O19 Formula weight 1171.35 Temperature 100(2) K Wavelength 1.54184 Å Crystal system Triclinic Space group Unit cell dimensions a = 13.8753(9) Å b = 15.3332(10) Å c = 16.1724(11) Å a= 83.896(5)° b= 69.456(6)° g = 74.517(6)° Volume 3104.7(4) Å3 Z 2 Density (calculated) 1.253 Mg/m3 μ 0.768 mm-1 F(000) 1260 Crystal size 0.43 x 0.24 x 0.04 mm3 θ range for data collection 2.918 to 67.315°. Index ranges -16<=h<=8, -18<=k<=18, -19<=l<=19 Reflections collected 26248 Independent reflections 10964 [R(int) = 0.0689] Completeness to θ = 67.315° 98.3 % Absorption correction Semi-empirical from equivalents Max./min. transmission 1.00/0.553 Refinement method Full-matrix least-squares on F2 Data / restraints / parameters 10964 / 42 / 818 Goodness-of-fit on F2 0.957 Final R indices [I>2σ(I)] R1 = 0.0990, wR2 = 0.2630 R indices (all data) R1 = 0.1573, wR2 = 0.3075 Largest diff. peak and hole 0.718 and -0.633 e.Å-3 Table S3. Hydrogen bonds for L·3H2O [Å and °].
____________________________________________________________________________
D-H...A d(D-H) d(H...A) d(D...A) <(DHA)
____________________________________________________________________________
N(232)-H(232)...O(23) 0.88 2.12 2.571(5) 110.7
O(234)-H(234)...O(332)1 0.84 2.22 2.600(7) 107.5
N(432)-H(432)...O(135)2 0.88 2.65 3.315(15) 132.9
O(1)-H(1B)...O(232) 0.84 2.12 2.689(10) 124.3
O(1)-H(1A)...O(3)3 0.84 1.82 2.595(16) 153.4
____________________________________________________________________________
Symmetry transformations used to generate equivalent atoms: 1 x,y,z+1; 2 1-x,1-y,-z; 3 -x,1-y,1-z
1P
Additional details for the structure of CaL
Table S4. Selected bond lengths [Å] and angles [°] for CaL.
_____________________________________________________
Ca(1)-O(132)1 2.270(3)
Ca(1)-O(51) 2.274(3)
Ca(1)-O(432) 2.298(3)
Ca(1)-O(1) 2.332(4)
Ca(1)-O(232)2 2.332(3)
Ca(1)-O(5) 2.366(3)
O(132)1-Ca(1)-O(51) 107.32(11)
O(132)1-Ca(1)-O(432) 163.60(12)
O(51)-Ca(1)-O(432) 86.60(10)
O(132)1-Ca(1)-O(1) 91.41(17)
O(51)-Ca(1)-O(1) 85.58(14)
O(432)-Ca(1)-O(1) 98.44(16)
O(132)1-Ca(1)-O(232)2 86.30(10)
O(51)-Ca(1)-O(232)2 159.01(12)
O(432)-Ca(1)-O(232)2 82.99(9)
O(1)-Ca(1)-O(232)2 78.02(14)
O(132)1-Ca(1)-O(5) 88.25(13)
O(51)-Ca(1)-O(5) 104.33(12)
O(432)-Ca(1)-O(5) 79.73(12)
O(1)-Ca(1)-O(5) 169.71(15)
O(232)2-Ca(1)-O(5) 91.70(11)
_____________________________________________________________
Symmetry transformations used to generate equivalent atoms:
1 -x,1-y,1-z; 2 x-1,y-1,z
Table S5. Hydrogen bonds for CaL [Å and °].
____________________________________________________________________________
D-H...A d(D-H) d(H...A) d(D...A) <(DHA)
____________________________________________________________________________
N(132)-H(132)...O(25) 0.88 2.31 3.066(14) 143.5
N(135)-H(135)...O(25) 0.88 2.31 2.987(11) 133.8
N(232)-H(232)...O(641)2 0.88 2.30 3.009(4) 138.0
N(332)-H(332)...O(33) 0.88 2.07 2.528(5) 111.6
N(332)-H(332)...O(61)2 0.88 2.29 3.106(6) 154.8
O(334)-H(334)...O(1)2 0.84 2.17 2.764(7) 128.1
O(434)-H(434)...O(621)3 0.84 2.34 3.124(4) 155.1
O(5)-H(5)...O(3)1 0.95 1.89 2.811(6) 162.2
O(6)-H(6)...O(61) 0.84 1.92 2.658(4) 146.5
O(6)-H(6)...O(621) 0.84 2.38 3.019(4) 133.9
O(7)-H(7)...O(434) 0.84 2.00 2.817(4) 165.7
____________________________________________________________________________
Symmetry transformations used to generate equivalent atoms:
1 x-1,y-1,z; 2 x+1,y,z; 3 -x,1-y,2-z
Additional details for the structure of LaL
Table S6. Selected bond lengths [Å] and angles [°] for LaL.
_____________________________________________________
La(1)-O(432) 2.465(3)
La(1)-O(332)1 2.465(3)
La(1)-O(51) 2.479(3)
La(1)-O(232)2 2.488(3)
La(1)-O(1) 2.537(3)
La(1)-O(3) 2.567(3)
La(1)-O(4) 2.574(3)
La(1)-O(2) 2.607(3)
La(1)-O(521) 2.710(3)
O(432)-La(1)-O(332)1 143.99(9)
O(432)-La(1)-O(51) 73.66(8)
O(332)1-La(1)-O(51) 126.18(9)
O(432)-La(1)-O(232)2 85.40(9)
O(332)1-La(1)-O(232)2 89.87(9)
O(51)-La(1)-O(232)2 140.86(9)
O(432)-La(1)-O(1) 138.57(11)
O(332)1-La(1)-O(1) 71.17(11)
O(51)-La(1)-O(1) 104.25(10)
O(232)2-La(1)-O(1) 70.54(11)
O(432)-La(1)-O(3) 86.09(10)
O(332)1-La(1)-O(3) 74.03(10)
O(51)-La(1)-O(3) 73.82(10)
O(232)2-La(1)-O(3) 138.32(10)
O(1)-La(1)-O(3) 134.07(11)
O(432)-La(1)-O(4) 70.12(9)
O(332)1-La(1)-O(4) 74.59(9)
O(51)-La(1)-O(4) 128.04(10)
O(232)2-La(1)-O(4) 70.92(11)
O(1)-La(1)-O(4) 127.56(11)
O(3)-La(1)-O(4) 67.81(10)
O(432)-La(1)-O(2) 71.88(10)
O(332)1-La(1)-O(2) 242.07(10)
O(51)-La(1)-O(2) 66.09(10)
O(232)2-La(1)-O(2) 76.19(10)
O(1)-La(1)-O(2) 69.92(12)
O(3)-La(1)-O(2) 138.14(10)
O(4)-La(1)-O(2) 130.91(10)
O(432)-La(1)-O(521) 133.46(8)
O(332)1-La(1)-O(521) 68.15(8)
O(51)-La(1)-O(521) 61.25(8)
O(232)2-La(1)-O(521) 137.67(9)
O(1)-La(1)-O(521) 68.27(10)
O(3)-La(1)-O(521) 71.52(9)
O(4)-La(1)-O(521) 130.59(9)
O(2)-La(1)-O(521) 98.19(10)
C(332)-O(332)-La(1)3 156.8(3)
C(232)-O(232)-La(1)4 148.2(3)
C(432)-O(432)-La(1) 145.5(2)
C(51)-O(51)-La(1) 145.7(2)
N(52)-O(521)-La(1) 144.6(2)
_____________________________________________________________
Symmetry transformations used to generate equivalent atoms: 1 x-1/2,-y+1/2,z-1/2; 2 x,y,z-1; 3 x+1/2,-y+1/2,z+1/2 ; 4 x,y,z+1
Table S7. Hydrogen bonds for LaL [Å and °].
____________________________________________________________________________
D-H...A d(D-H) d(H...A) d(D...A) <(DHA)
____________________________________________________________________________
N(132)-H(132)...O(25) 0.88 2.16 2.963(4) 150.6
O(134)-H(134)...O(61) 0.833(14) 1.77(2) 2.576(4) 164 (5)
O(134)-H(134)...O(661) 0.833(14) 2.46(5) 2.953(5) 119(4)
N(232)-H(232)...O(35) 0.88 2.19 2.974(4) 148.2
O(234)-H(234)...O(5) 0.84 2.27 2.901(5) 132.2
N(332)-H(332)...O(45) 0.88 2.36 3.116(5) 144.0
O(334)-H(334)...O(134)3 0.844(14) 2.07(4) 2.716(5) 132(5)
N(432)-H(432)...O(43) 0.88 2.10 2.547(4) 110.7
O(434)-H(434)...O(561)4 0.84 2.36 3.074(14) 143.1
O(435)-H(435)...O(5)2 0.84 2.36 2.848(11) 117.9
O(1)-H(1AO)...O(334)1 0.849(18) 2.22(3) 2.995(5) 151(4)
O(1)-H(1BO)...O(71) 0.815(18) 2.01(3) 2.760(5) 153(5)
O(1)-H(1BO)...O(761) 0.815(18) 2.32(4) 2.924(4) 131(5)
O(2)-H(2AO)...O(561) 0.820(18) 2.18(2) 2.999(5) 177(5)
O(3)-H(3BO)...O(621)3 0.819(18) 2.20(3) 2.968(4) 157(4)
O(4)-H(4AO)...O(132)3 0.841(19) 2.14(3) 2.937(4) 157(5)
O(4)-H(4BO)...O(5)2 0.847(19) 1.90(3) 2.711(5) 161(5)
____________________________________________________________________________
Symmetry transformations used to generate equivalent atoms: 1 x-1/2,-y+1/2,z-1/2 ; 2 x,y,z-1 ; 3 x+1/2,-y+1/2,z-1/2; 4 -x,-y,-z
Additional details for the structure of PrL
Fig S4 Molecular structure of PrL. Hydrogen atoms and the minor components of the disordered atoms have been omitted. Ellipsoids have been drawn at the 50% probability level.
Table S8. Selected bond lengths [Å] and angles [°] for PrL.
_____________________________________________________
Pr(1)-O(232)1 2.3872(16)
Pr(1)-O(432) 2.4050(19)
Pr(1)-O(61) 2.4192(15)
Pr(1)-O(51) 2.4226(17)
Pr(1)-O(132)2 2.4492(19)
Pr(1)-O(1) 2.493(2)
Pr(1)-O(5) 2.527(2)
Pr(1)-O(621) 2.5848(17)
Pr(1)-O(521) 2.700(2)
O(232)1-Pr(1)-O(432) 76.23(6)
O(232)1-Pr(1)-O(61) 142.95(6)
O(432)-Pr(1)-O(61) 70.97(6)
O(232)1-Pr(1)-O(51) 132.90(6)
O(432)-Pr(1)-O(51) 142.43(7)
O(61)-Pr(1)-O(51) 72.85(6)
O(232)1-Pr(1)-O(132)2 80.18(6)
O(432)-Pr(1)-O(132)2 139.57(9)
O(61)-Pr(1)-O(132)2 136.68(6)
O(51)-Pr(1)-O(132)2 76.27(7)
O(232)1-Pr(1)-O(1) 79.29(7)
O(432)-Pr(1)-O(1) 76.64(9)
O(61)-Pr(1)-O(1) 76.84(7)
O(51)-Pr(1)-O(1) 85.66(8)
O(132)2-Pr(1)-O(1) 130.19(9)
O(232)1-Pr(1)-O(5) 72.74(7)
O(432)-Pr(1)-O(5) 72.61(10)
O(61)-Pr(1)-O(5) 112.02(7)
O(51)-Pr(1)-O(5) 131.96(8)
O(132)2-Pr(1)-O(5) 69.24(9)
O(1)-Pr(1)-O(5) 142.33(9)
O(232)1-Pr(1)-O(621) 140.33(5)
O(432)-Pr(1)-O(621) 100.05(7)
O(61)-Pr(1)-O(621) 64.04(5)
O(51)-Pr(1)-O(621) 72.45(6)
O(132)2-Pr(1)-O(621) 78.19(6)
O(1)-Pr(1)-O(621) 139.15(7)
O(5)-Pr(1)-O(621) 68.62(6)
O(232)1-Pr(1)-O(521) 69.59(6)
O(432)-Pr(1)-O(521) 132.03(8)
O(61)-Pr(1)-O(521) 122.70(6)
O(51)-Pr(1)-O(521) 63.61(6)
O(132)2-Pr(1)-O(521) 65.45(8)
O(1)-Pr(1)-O(521) 64.92(8)
O(5)-Pr(1)-O(521) 124.52(8)
O(621)-Pr(1)-O(521) 127.73(6)
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Symmetry transformations used to generate equivalent atoms: 1 x+1,y+1,z; 2 1-x,2-y,2-z
Table S9. Hydrogen bonds for PrL [Å and °].
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D-H...A d(D-H) d(H...A) d(D...A) <(DHA)
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N(132)-H(132)...O(25) 0.88 2.24 3.046(3) 152.3
N(232)-H(232)...O(6) 0.88 2.11 2.818(3) 136.4
O(234)-H(234)...O(332)3 0.84 1.89 2.722(3) 170.3
C(251)-H(25C)...O(522)2 0.98 2.59 3.521(4) 158.3
N(332)-H(332)...O(45) 0.88 2.55 3.356(3) 152.3
O(334)-H(334)...O(741) 0.84 2.32 3.038(10) 143.4
O(334)-H(334)...O(861) 0.84 2.51 3.21(3) 142.2
O(334)-H(334)...O(862) 0.84 2.51 3.331(9) 165.3
O(334)-H(334)...O(2) 0.84 2.59 3.204(12) 130.7
N(432)-H(432)...O(722) 0.88 2.27 3.049(7) 146.8
N(435)-H(43H)...O(437) 0.88 2.30 2.72(3) 109.4
O(5)-H(5O)...O(234)1 0.95 2.06 2.736(3) 126.3
O(6)-H(6O)...O(71)4 0.84 1.72 2.556(5) 171.8
O(6)-H(6O)...O(822)4 0.84 2.57 3.287(15) 143.8
O(7)-H(7)...O(841) 0.84 2.53 3.09(2) 124.3
O(7)-H(7)...O(842) 0.84 2.02 2.818(16) 158.4
O(7)-H(7)...O(8)5 0.84 1.86 2.651(8) 157.4
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Symmetry transformations used to generate equivalent atoms: 1 x+1,y+1,z; 2 x-1,y-1,z; 3 1-x,1-y,2-z; 4 1-x,1-y,1-z; 5 2-x,2-y,1-z
Additional details for the structure of YbL
Table S10. Selected bond lengths [Å] and angles [°] for YbL.
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Yb(1)-O(71) 2.20(5)
Yb(1)-O(61) 2.230(6)
Yb(1)-O(232)1 2.236(5)
Yb(1)-O(432) 2.256(6)
Yb(1)-O(132)2 2.257(6)
Yb(1)-O(1) 2.275(7)
Yb(1)-O(81) 2.32(5)
Yb(1)-O(721) 2.38(2)
Yb(1)-O(661) 2.497(6)
Yb(1)-O(821) 2.52(2)
O(71)-Yb(1)-O(61) 81.6(13)
O(71)-Yb(1)-O(232)1 107.9(16)
O(61)-Yb(1)-O(232)1 143.9(2)
O(71)-Yb(1)-O(432) 141.5(11)
O(61)-Yb(1)-O(432) 73.9(2)
O(232)1-Yb(1)-O(432) 78.2(2)
O(71)-Yb(1)-O(132)2 73.5(11)
O(61)-Yb(1)-O(132)2 137.3(2)
O(232)1-Yb(1)-O(132)2 77.9(2)
O(432)-Yb(1)-O(132)2 142.9(3)
O(71)-Yb(1)-O(1) 139.5(13)
O(61)-Yb(1)-O(1) 105.6(3)
O(232)1-Yb(1)-O(1) 89.7(3)
O(432)-Yb(1)-O(1) 76.8(2)
O(132)2-Yb(1)-O(1) 75.1(3)
O(61)-Yb(1)-O(81) 76.6(13)
O(232)1-Yb(1)-O(81) 109.9(15)
O(432)-Yb(1)-O(81) 135.7(11)
O(132)2-Yb(1)-O(81) 79.5(11)
O(1)-Yb(1)-O(81) 143.7(13)
O(71)-Yb(1)-O(721) 67.4(15)
O(61)-Yb(1)-O(721) 79.7(6)
O(232)1-Yb(1)-O(721) 72.8(6)
O(432)-Yb(1)-O(721) 79.1(6)
O(132)2-Yb(1)-O(721) 119.6(6)
O(1)-Yb(1)-O(721) 152.7(6)
O(71)-Yb(1)-O(661) 75.8(16)
O(61)-Yb(1)-O(661) 67.2(2)
O(232)1-Yb(1)-O(661) 148.5(2)
O(432)-Yb(1)-O(661) 119.1(2)
O(132)2-Yb(1)-O(661) 73.3(2)
O(1)-Yb(1)-O(661) 71.0(2)
O(81)-Yb(1)-O(661) 77.1(15)
O(721)-Yb(1)-O(661) 133.3(6)
O(61)-Yb(1)-O(821) 72.9(6)
O(232)1-Yb(1)-O(821) 76.9(6)
O(432)-Yb(1)-O(821) 72.0(5)
O(132)2-Yb(1)-O(821) 128.4(5)
O(1)-Yb(1)-O(821) 147.9(6)
O(81)-Yb(1)-O(821) 68.1(14)
O(661)-Yb(1)-O(821) 131.8(6)
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Symmetry transformations used to generate equivalent atoms: 1 x,y-1,z ; 2 1-x,1-y,1-z
1 Sheldrick, G.M. (2015). Acta Cryst. C71, 3-8